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<ep-patent-document id="EP05736848B1" file="EP05736848NWB1.xml" lang="en" country="EP" doc-number="1742758" kind="B1" date-publ="20080109" status="n" dtd-version="ep-patent-document-v1-2">
<SDOBI lang="en"><B000><eptags><B001EP>ATBECHDEDKESFRGBGRITLILUNLSEMCPTIESILT..FIRO..CY..TRBGCZEEHUPLSK....IS..........</B001EP><B003EP>*</B003EP><B005EP>J</B005EP><B007EP>DIM360 Ver 2.4  (29 Nov 2007) -  2100000/0</B007EP></eptags></B000><B100><B110>1742758</B110><B120><B121>EUROPEAN PATENT SPECIFICATION</B121></B120><B130>B1</B130><B140><date>20080109</date></B140><B190>EP</B190></B100><B200><B210>05736848.2</B210><B220><date>20050418</date></B220><B240><B241><date>20060915</date></B241></B240><B250>en</B250><B251EP>en</B251EP><B260>en</B260></B200><B300><B310>832640</B310><B320><date>20040426</date></B320><B330><ctry>US</ctry></B330></B300><B400><B405><date>20080109</date><bnum>200802</bnum></B405><B430><date>20070117</date><bnum>200703</bnum></B430><B450><date>20080109</date><bnum>200802</bnum></B450><B452EP><date>20070730</date></B452EP></B400><B500><B510EP><classification-ipcr sequence="1"><text>B23K  26/40        20060101AFI20051121BHEP        </text></classification-ipcr><classification-ipcr sequence="2"><text>B23K  26/42        20060101ALI20051121BHEP        </text></classification-ipcr><classification-ipcr sequence="3"><text>B23K  26/06        20060101ALI20051121BHEP        </text></classification-ipcr><classification-ipcr sequence="4"><text>B01J  19/12        20060101ALI20051121BHEP        </text></classification-ipcr><classification-ipcr sequence="5"><text>H01L  21/268       20060101ALI20051121BHEP        </text></classification-ipcr></B510EP><B540><B541>de</B541><B542>VERFAHREN UND EINRICHTUNG ZUM LASERÄTZEN EINER STRUKTUR DURCH ZUNÄCHST BESTRAHLEN VON BEREICHEN DER STRUKTUR ZUR ÄNDERUNG DER KRISTALLINITÄT</B542><B541>en</B541><B542>A METHOD OF AND AN ARRANGEMENT FOR LASER ETCHING A STRUCTURE BY FIRST RADIATING AREAS OF THE STRUCTURE FOR ALTERING THE CRYSTALLINITY</B542><B541>fr</B541><B542>PROCEDE ET ARRANGEMENT DE GRAVURE LASER D'UNE STRUCTURE COMMENÇANT PAR L'IRRADIATION DE ZONES DE CETTE STRUCTURE AFIN D'EN MODIFIER LA CRISTALLINITE</B542></B540><B560><B561><text>EP-A- 1 067 593</text></B561><B561><text>US-A- 4 834 834</text></B561><B561><text>US-A- 4 877 939</text></B561><B561><text>US-A- 4 961 052</text></B561><B561><text>US-A- 5 024 724</text></B561><B561><text>US-A- 5 580 473</text></B561><B561><text>US-A1- 2002 017 116</text></B561><B561><text>US-B1- 6 617 541</text></B561></B560></B500><B700><B720><B721><snm>NELSON, Curt</snm><adr><str>1000 NE Circle Blvd.</str><city>Corvallis, Oregon 97330</city><ctry>US</ctry></adr></B721><B721><snm>LONG, Greg</snm><adr><str>1000 NE Circle Blvd.</str><city>Corvallis, Oregon 97330</city><ctry>US</ctry></adr></B721></B720><B730><B731><snm>Hewlett-Packard Development Company, L.P.</snm><iid>07151750</iid><irf>HP050405PEP</irf><adr><str>Hewlett-Packard Company 
I. P. Admin., 20555 S.H. 249</str><city>Houston, TX 77070</city><ctry>US</ctry></adr></B731></B730><B740><B741><snm>Schoppe, Fritz</snm><sfx>et al</sfx><iid>00055463</iid><adr><str>Schoppe, Zimmermann, Stöckeler &amp; Zinkler 
Patentanwälte 
Postfach 246</str><city>82043 Pullach bei München</city><ctry>DE</ctry></adr></B741></B740></B700><B800><B840><ctry>AT</ctry><ctry>BE</ctry><ctry>BG</ctry><ctry>CH</ctry><ctry>CY</ctry><ctry>CZ</ctry><ctry>DE</ctry><ctry>DK</ctry><ctry>EE</ctry><ctry>ES</ctry><ctry>FI</ctry><ctry>FR</ctry><ctry>GB</ctry><ctry>GR</ctry><ctry>HU</ctry><ctry>IE</ctry><ctry>IS</ctry><ctry>IT</ctry><ctry>LI</ctry><ctry>LT</ctry><ctry>LU</ctry><ctry>MC</ctry><ctry>NL</ctry><ctry>PL</ctry><ctry>PT</ctry><ctry>RO</ctry><ctry>SE</ctry><ctry>SI</ctry><ctry>SK</ctry><ctry>TR</ctry></B840><B860><B861><dnum><anum>US2005013180</anum></dnum><date>20050418</date></B861><B862>en</B862></B860><B870><B871><dnum><pnum>WO2005108000</pnum></dnum><date>20051117</date><bnum>200546</bnum></B871></B870><B880><date>20070117</date><bnum>200703</bnum></B880></B800></SDOBI><!-- EPO <DP n="1"> -->
<description id="desc" lang="en">
<p id="p0001" num="0001">The present application concerns a method of etching a structure and an arrangement with an etching system and a structure according to the preamble of, respectively, claims 1 and 10 (see, for example, <patcit id="pcit0001" dnum="US4961052A"><text>US-A-4 961 052</text></patcit>).</p>
<heading id="h0001">BACKGROUND</heading>
<p id="p0002" num="0002">Etching is the process of removing material from selected areas. The etching process may be used for several applications. For example, etching may be used in precise patterning of traces and other intricate features on electronic devices. Those patterned traces, among other things, allow electronic devices to work.</p>
<p id="p0003" num="0003">In the past, etching has been accomplished using wet etching or dry etching techniques. Both wet and dry etching techniques, however, may involve complicated machinery and chemical storage, handling, and disposal problems. Additionally, some of those techniques may excessively undercut the area being etched leading to less than precise etching.</p>
<p id="p0004" num="0004"><patcit id="pcit0002" dnum="US4834834A"><text>US -A-4834834</text></patcit> discloses a method of patterning a layered article comprising using a first laser beam to create a chemical reaction of the article with a halogen atmosphere, except at selected areas, and then using a second laser beam to ablate the surface of the article, except at the same selected areas.</p>
<p id="p0005" num="0005"><patcit id="pcit0003" dnum="US4961052A"><text>US-A-4961052</text></patcit> discloses an etching method for a photosensitive glass substrate which is masked and then exposed to UV radiation. The exposed portions are crystallised and subsequently removed by acid. According to a first aspect of the present invention, a method of etching a structure is defined in claim 1.<!-- EPO <DP n="2"> --></p>
<p id="p0006" num="0006">According to a second aspect of the present invention, an arrangement comprising an etching system and a structure is defined in claim 10.</p>
<heading id="h0002">BRIEF DESCRIPTION OF THE DRAWINGS</heading>
<p id="p0007" num="0007">
<ul id="ul0001" list-style="none" compact="compact">
<li>Fig. 1 is a schematic view illustrating operation of an embodiment of a selective etching system, according to an embodiment of the invention.</li>
<li>Fig. 2 is a schematic view illustrating operation of an embodiment of an electromagnetic radiation system forming a part of an embodiment of a selective etching system constructed in accordance with another embodiment of the invention.</li>
<li>Fig. 3 is a schematic view illustrating operation of the embodiment of the first electromagnetic radiation system forming a part of an embodiment of a selective etching system constructed In accordance with yet another embodiment of the invention.</li>
<li>Fig. 4 is a schematic diagram illustrating a change of crystallinity and order state of a material upon melting the material and recrystallizing the materiel according to one embodiment.<!-- EPO <DP n="3"> --></li>
<li>Fig. 5 is a flowchart illustrating an example of a selective etching method not covered by the invention as defined in the appended claims.</li>
</ul></p>
<heading id="h0003">DETAILED DESCRIPTION</heading>
<p id="p0008" num="0008">Referring initially to Fig. 1, an embodiment of a selective etching system is shown schematically at 10, the system including a first electromagnetic radiation system 20 and a second electromagnetic radiation system 30. Although two distinct electromagnetic radiation systems are shown, it will be appreciated that the depicted electromagnetic radiation systems are intended to illustrate different electromagnetic radiation operations, whether or not different systems are employed. Through the indicated electromagnetic radiation operations, a characteristic of structure 40 may be altered in an area, such as target area 42, of the structure, and the structure may be selectively ablated based on that characteristic.</p>
<p id="p0009" num="0009">As indicated, selective etching system 10 may be employed to define a trace on structure 40, such as that shown at 44 in Fig. 1. Structure 40 may be formed of virtually any material or combination of materials that may be altered chemically and/or physically by selective etching system 10. For example, structure 40 may take the form of a silicon substrate 40<u style="single">a,</u> having a surface layer 40b. Such a structure may be etched to define precise traces and other intricate features, which may be used for electrical connections in electronic devices.</p>
<p id="p0010" num="0010">Surface layer 40b may be defined by a thin film overlying structure 40 or may be formed integrally with that structure. The depth of surface layer 40b may correspond to the desired depth of etching by selective etching system 10 and may be formed with a characteristic alterable upon application of electromagnetic radiation from one or more electromagnetic radiation systems.</p>
<p id="p0011" num="0011">It will be appreciated that although the exemplary surface layer is described as being formed of amorphous silicon, the surface layer may be formed of virtually any material configurable for selected ablation based on a characteristic alterable by application of electromagnetic radiation. The surface layer may be composed of the same material as structure 40 or may be composed of a different material than that structure. For example, structure 40 may be a silicon substrate and surface layer 40b may be a thin film of amorphous<!-- EPO <DP n="4"> --> silicon. The amorphous silicon surface layer may have a thickness of 25 to 400 nanometers, which corresponds to the desired depth of etching.</p>
<p id="p0012" num="0012">As indicated, a mask 50 may be introduced between first electromagnetic radiation system 20 and structure 40, the mask defining a pattern 52 corresponding to a desired etch. Upon applying electromagnetic radiation, such as via laser beam 24 in Fig. 1, the mask may shield a non-target area 46 on the structure but allow application of the electromagnetic radiation to target area 42 on the structure. As shown, target area 42 generally corresponds to pattern 52 of mask 50. The pattern thus may be projected onto surface layer 40<u style="single">b</u> of structure 40 to define a desired etch on the surface layer by scanning laser beam 24 across mask 50.</p>
<p id="p0013" num="0013">Alternatively, or additionally, a galvo head system 60 may be placed between first electromagnetic radiation system 20 and structure 40, to selectively direct first electromagnetic radiation to the structure. Upon applying electromagnetic radiation, such as via laser beam 24 in Fig. 2, the galvo head system may, by employing one or more reflectors 62, direct the application of the electromagnetic radiation to target area 42 without the application of electromagnetic radiation to non-target area 46. Galvo head system 60 may include various componentry to selectively move reflectors 62, which may include servo motors and control software (not shown).</p>
<p id="p0014" num="0014">As indicated in Fig. 3, structure 40 may, alternatively or additionally, be located on a stage 70 to allow the structure to be moved thereby selectively directing first electromagnetic radiation to structure 40. Upon applying electromagnetic radiation, such as via laser beam 24 in Fig. 3, the stage may move structure 40 to direct the application of the electromagnetic radiation to target area 42 without the application of that radiation to non-target area 46. Stage 70 may include various componentry to selectively move structure 40, which may include any suitable motor and control software (not shown). It will be appreciated that although an exemplary galvo head system and stage are described, the disclosure includes virtually any system or device configured to selectively direct first electromagnetic radiation to target area 42 by redirecting the first electromagnetic radiation and/or moving the structure.<!-- EPO <DP n="5"> --></p>
<p id="p0015" num="0015">In accordance with the present teachings, surface layer 40b may have one or more characteristics that are altered upon application of selected electromagnetic radiation. Such characteristic may include virtually any suitable chemical, physical, or other property. One such alterable characteristic is crystallinity (or order state).</p>
<p id="p0016" num="0016">Crystallinity, as used herein, refers to the size of crystals in structure 40. Order state, as used herein, refers to the state of arrangement of atoms, ions, molecules and/or particles of structure 40, and may range from a generally random, less-ordered state to a generally predictable, more-ordered state. Accordingly, as will be described further below, upon application of laser beam 24 to target area 42 of structure 40, crystallinity (or order state) of the structure in the target area may be altered relative to the crystallinity (or order state) of structure in the non-target area shielded by mask 50.</p>
<p id="p0017" num="0017">First electromagnetic radiation system 20 may be configured to direct electromagnetic radiation at target area 42 of structure 40 to alter the crystallinity (or order state) in that area. The first electromagnetic radiation system may provide virtually any form of electromagnetic radiation. As shown in Fig. 1, first electromagnetic radiation system 20 may include a first laser 22 configured to direct laser beam 24 with photons (continuously or in laser beam pulses) at target area 42. The first laser may take the form of virtually any gas, liquid or solid-state laser, or any other source, configured to change crystallinity and/or order state of target area 42 of structure 40.</p>
<p id="p0018" num="0018">First laser 22 may be an ultraviolet (UV) laser that provides a homogenized excimer laser beam configured to change crystallinity and/or order state of target area 42 of structure 40. UV laser, as used herein, refers to a laser that provides a laser beam in the ultraviolet wavelength range of approximately 100 to 400 nanometers. Other types of lasers may be used that provide a laser beam in different wavelength ranges. Typically, where structure 40 is formed of silicon as described above, first laser 22 provides a laser beam in the wavelength range of 200 to 850 nanometers to change crystallinity and/or order state of target area 42 of structure 40.<!-- EPO <DP n="6"> --></p>
<p id="p0019" num="0019">The fluence, pulse length, and/or other suitable operational parameters of first laser 22 may be adjusted to achieve the desired change of crystallinity and/or order state of target area 42 of structure 40. Fluence, as used herein, refers to the number of photons per unit area, per unit time. Pulse length or pulse duration, as used herein, refers to the lifetime of the laser beam pulse expressed in units of time. Typically, the fluence, pulse length, and/or other suitable operational parameters of first laser 22 are chosen to be sufficient to achieve the desired change of crystallinity and/or order state of target area 42 but insufficient to ablate that area. For example, first laser 22 may be configured to have a fluence of 300 to 700 millijoules per square centimeter (mJ/cm<sup>2</sup>), and a pulse length of 5 to 50 nanoseconds to melt the surface layer of structure formed of silicon such as that described above. Upon being melted, the surface layer may be allowed to recrystallize into the desired crystallinity and/or order state.</p>
<p id="p0020" num="0020">Second electromagnetic radiation system 30 may be configured to direct electromagnetic radiation at structure 40 and selectively ablate the surface layer of that structure based on the difference in crystallinity (or order state) between target area 42 and non-target area 46. The second electromagnetic radiation system may provide virtually any form of electromagnetic radiation. In Fig. 1, for example, second electromagnetic radiation system 30 may include a second laser 32 configured to direct a laser beam 34 with photons (continuously or in laser beam pulses) at surface layer 40<u style="single">b</u> of structure 40. The second laser may take the form of virtually any gas, liquid, and/or solid-state laser, or any other source, configured to selectively ablate surface layer 40<u style="single">b</u> that layer based on differences in crystallinity and/or order state.</p>
<p id="p0021" num="0021">Second laser 32 may be a neodymium: yttrium-aluminum garnet (YAG) laser configured to selectively ablate surface layer 40<u style="single">b</u> of structure 40 based on differences in crystallinity and/or order state. YAG laser, as used herein, refers to a solid-state laser that uses yttrium aluminum garnet doped with neodymium as the matrix material. Other types of lasers may be used that provide a laser beam in different wavelength ranges, such as lasers that provide a laser beam in the wavelength range of 300 to 750 nanometers to selectively ablate the surface layer.<!-- EPO <DP n="7"> --></p>
<p id="p0022" num="0022">The fluence, pulse length, and/or other suitable operational parameters of second laser 32 also is adjusted to ablate the surface layer in non-target area 46, but not ablate the surface layer in target area 42. Where the surface layer is formed of silicon, as described above, second laser 46 may be adjusted to have a fluence of 500 to 2500 mJ/cm<sup>2</sup>, and a pulse length of 5 to 50 nanoseconds to ablate non-target area 46 of structure 40. A trace 44 thus may be left on structure 40, as shown in Fig. 1.</p>
<p id="p0023" num="0023">It will be appreciated that although exemplary electromagnetic radiation systems are described as including lasers, the systems may include any form of electromagnetic radiation source configurable for altering one or more characteristics of target area 42 of structure 40 and/or selectively ablating structure 40 based on those altered characteristics. The systems may be composed of the same type of electromagnetic radiation source or may be composed of different types of electromagnetic radiation sources.</p>
<p id="p0024" num="0024">The effects first laser 22 may have on target area 42 are schematically illustrated in Fig. 4. In some embodiments, surface layer 40<u style="single">b</u> of structure 40 may be formed of relatively small crystals 48a before melting by first laser 22. After allowing the melted surface layer to recrystallize, that layer in target area 42 may be formed of relatively large crystals 48<u style="single">b</u>. Similarly, first laser 22 may effect a transformation of the surface layer in target area 42 from a generally random, less-ordered state 49<u style="single">a</u> to a generally predictable, more-ordered state 49<u style="single">b.</u> Although only increases of crystal size and order state are illustrated, the scope of the disclosure includes first laser 22 having the effect of decreasing crystal size and/or order state.</p>
<p id="p0025" num="0025">The change of crystallinity and/or order state allows second laser 32 to selectively ablate non-target area 46 based on the difference of characteristics between target and non-target areas. For example, increasing crystal size in target area 42 may make target area 42 more resistant to laser ablation. Thus, the fluence and/or other suitable operational parameters of second laser 32 are chosen to be sufficient to ablate non-target area 46 but not sufficient to ablate target area 42. It will be appreciated that although the<!-- EPO <DP n="8"> --> effects of the first laser are illustrated only in connection with crystallinity and order state, the scope of the disclosure may include other effects of the first laser.</p>
<p id="p0026" num="0026">Fig. 5 is a flowchart 100 illustrating an example of a selective etching method not covered by the invention as defined in the appended claims. At 102, a first electromagnetic radiator system is configured such that electromagnetic radiation is applied only to a target area. For example, a mask is used to shield a non-target area 46. At 104, electromagnetic radiation from a first electromagnetic radiation system is applied to the target area 42 of structure. For example, a UV laser beam may be applied to the target area of the structure. At 106, one or more characteristics of surface layer in the target area of the structure are changed by application of the electromagnetic radiation. Accordingly, the surface layer in the target area of the structure may be melted by the application of electromagnetic radiation.</p>
<p id="p0027" num="0027">At 108, the one or more characteristics that were changed by application of electromagnetic radiation are allowed to stabilize resulting in a surface layer with a differential surface characteristic. In particular, a melted surface layer may be allowed to recrystallize to define a surface layer with a differential surface characteristic. At 110, electromagnetic radiation from a second electromagnetic radiation system may be applied to the surface layer. For example, a YAG laser beam may be applied to the surface layer. At 112, the surface layer may be selectively ablated by the second electromagnetic radiation system based on the differential surface characteristic. Accordingly, the recrystallized surface layer may be selectively ablated by the YAG laser beam based on differential surface characteristic.</p>
<p id="p0028" num="0028">Although the present embodiments have been shown and described, it will be apparent to those skilled in the art that various changes in form and detail may be made without departing from the scope defined in the appended claims. The present disclosure is intended to embrace all such alternatives, modifications, and variances. Where the disclosure or claims recite "a," "a first," or "another" element, or the equivalent thereof, they should be interpreted to include one or more such elements, neither requiring nor excluding two or more such elements.</p>
</description><!-- EPO <DP n="9"> -->
<claims id="claims01" lang="en">
<claim id="c-en-01-0001" num="0001">
<claim-text>A method of etching a structure (40) comprising : applying a first electromagnetic radiation (24) to a first area (42) of a structure (40) comprising first (42) and second (46) areas, thereby altering a physical characteristic of the structure (40) In the first area (42); <b>characterised by</b> applying a second electromagnetic radiation (34) to the second area (46) of the structure (40), the second electromagnetic radiation (34) being configured to selectively ablate the second area (46) of the structure (40).</claim-text></claim>
<claim id="c-en-01-0002" num="0002">
<claim-text>The method according to claim 1, wherein said alteration of a physical characteristic of the structure (40) comprises melting of the material in the first area (42) and, before the application of the second electromagnetic radiation (34), the material is allowed to stabilize.</claim-text></claim>
<claim id="c-en-01-0003" num="0003">
<claim-text>The method of claim 1, where the characteristic is crystallinity.</claim-text></claim>
<claim id="c-en-01-0004" num="0004">
<claim-text>The method of claim 3, where applying the first electromagnetic radiation (24) Includes melting a surface layer (40<u style="single">b</u>) in the area (42), and allowing the surface layer (40b) in the area (42) to recrystallize.</claim-text></claim>
<claim id="c-en-01-0005" num="0005">
<claim-text>The method of claim 1, where applying the first electromagnetic radiation (24) includes applying a first laser beam (24) with a fluence sufficient to melt a surface layer (40<u style="single">b</u>) of the structure (40) In the first area (42), but insufficient to ablate the surface layer (40<u style="single">b</u>) of the structure (40) in the first area (42).</claim-text></claim>
<claim id="c-en-01-0006" num="0006">
<claim-text>The method of claim 5, where applying the second electromagnetic radiation (34) includes applying a second laser beam (34) with a fluence sufficient to ablate the second area (46) of the surface layer (40<u style="single">b)</u><!-- EPO <DP n="10"> --> unmelted by the first laser beam (24), but insufficient to ablate the first area (42) of the surface layer (40b),</claim-text></claim>
<claim id="c-en-01-0007" num="0007">
<claim-text>The method of any preceding claim, comprising using a UV laser to apply to the first electromagnetic radiation (24),</claim-text></claim>
<claim id="c-en-01-0008" num="0008">
<claim-text>The method of any preceding claim, comprising using a YAG laser to apply the second electromagnetic radiation (34).</claim-text></claim>
<claim id="c-en-01-0009" num="0009">
<claim-text>The method of any preceding claim, wherein applying the first electromagnetic radiation (24) to the first area (42) includes placing a mask (50) intermediate the first electromagnetic radiation (24) and the structure (40), the mask (50) configured to shield the second area (46) of the structure (40) from the first electromagnetic radiation (24).</claim-text></claim>
<claim id="c-en-01-0010" num="0010">
<claim-text>An arrangement comprising an etching system (10) and a structure (40) which is of a material capable of being selectively etched by the system (10) and comprises first (42) and second (46) areas etching system (10), comprising: a first electromagnetic radiation source (20) configured to apply a first electromagnetic radiation (24) to the first area (42) of the structure (40), the first electromagnetic radiation (24) being selected to alter a characteristic of the first area (42); and <b>characterised by</b> a second electromagnetic radiation source (30) configured to apply a second electromagnetic radiation (34) to the second area (46) of the structure (40), the second electromagnetic radiation (34) being configured to selectively ablate the second area (46) of the structure (40).</claim-text></claim>
</claims><!-- EPO <DP n="11"> -->
<claims id="claims02" lang="de">
<claim id="c-de-01-0001" num="0001">
<claim-text>Ein Verfahren zum Ätzen einer Struktur (40), das folgende Schritte aufweist:
<claim-text>Anwenden einer ersten elektromagnetischen Strahlung (24) auf einen ersten Bereich (42) einer Struktur (40), die einen ersten (42) und einen zweiten (46) Bereich aufweist, wodurch eine physikalische Charakteristik der Struktur (40) in dem ersten Bereich (42) geändert wird;</claim-text>
<claim-text><b>gekennzeichnet durch</b> ein Anwenden einer zweiten elektromagnetischen Strahlung (34) auf den zweiten Bereich (46) der Struktur (40), wobei die zweite elektromagnetische Strahlung (34) konfiguriert wird, um den zweiten Bereich (46) der Struktur (40) selektiv abzutragen.</claim-text></claim-text></claim>
<claim id="c-de-01-0002" num="0002">
<claim-text>Das Verfahren gemäß Anspruch 1, bei dem die Änderung einer physikalischen Charakteristik der Struktur (40) ein Schmelzen des Materials in dem ersten Bereich (42) aufweist und vor der Anwendung der zweiten elektromagnetischen Strahlung (34) ermöglicht wird, dass sich das Material stabilisiert.</claim-text></claim>
<claim id="c-de-01-0003" num="0003">
<claim-text>Das Verfahren gemäß Anspruch 1, bei dem die Charakteristik eine Kristallinität ist.</claim-text></claim>
<claim id="c-de-01-0004" num="0004">
<claim-text>Das Verfahren gemäß Anspruch 3, bei dem das Anwenden der ersten elektromagnetischen Strahlung (24) ein Schmelzen einer Oberflächenschicht (40<u style="single">b</u>) in dem Bereich (42) und ein Ermöglichen, dass die Oberflächenschicht (40b) in dem Bereich (42) sich rekristallisiert, umfasst.<!-- EPO <DP n="12"> --></claim-text></claim>
<claim id="c-de-01-0005" num="0005">
<claim-text>Das Verfahren gemäß Anspruch 1, bei dem das Anwenden der ersten elektromagnetischen Strahlung (24) ein Anwenden eines ersten Laserstrahls (24) mit einer Fluenz umfasst, die ausreichend ist, um eine Oberflächenschicht (40<u style="single">b</u>) der Struktur (40) in dem ersten Bereich (42) zu schmelzen, aber nicht ausreichend ist, um die Oberflächenschicht (40<u style="single">b</u>) der Struktur (40) in dem ersten Bereich (42) abzutragen.</claim-text></claim>
<claim id="c-de-01-0006" num="0006">
<claim-text>Das Verfahren gemäß Anspruch 5, bei dem das Anwenden der zweiten elektromagnetischen Strahlung (34) ein Anwenden eines zweiten Laserstrahls (34) mit einer Fluenz umfasst, die ausreichend ist, um den zweiten Bereich (46) der Oberflächenschicht (40<u style="single">b</u>) abzutragen, der durch den ersten Laserstrahl (24) nicht geschmolzen ist, aber nicht ausreichend ist, um den ersten Bereich (42) der Oberflächenschicht (40b) abzutragen.</claim-text></claim>
<claim id="c-de-01-0007" num="0007">
<claim-text>Das Verfahren gemäß einem der vorhergehenden Ansprüche, das ein Verwenden eines UV-Lasers aufweist, um die erste elektromagnetische Strahlung (24) anzuwenden.</claim-text></claim>
<claim id="c-de-01-0008" num="0008">
<claim-text>Das Verfahren gemäß einem der vorhergehenden Ansprüche, das ein Verwenden eines YAG-Lasers aufweist, um die zweite elektromagnetische Strahlung (34) anzuwenden.</claim-text></claim>
<claim id="c-de-01-0009" num="0009">
<claim-text>Das Verfahren gemäß einem der vorhergehenden Ansprüche, bei dem das Anwenden der ersten elektromagnetischen Strahlung (24) auf den ersten Bereich (42) ein Platzieren einer Maske (50) zwischen der ersten elektromagnetischen Strahlung (24) und der Struktur (40) umfasst, wobei die Maske (50) konfiguriert wird, um den zweiten Bereich (46) der Struktur (40) von der ersten elektromagnetischen Strahlung (24) abzuschirmen.<!-- EPO <DP n="13"> --></claim-text></claim>
<claim id="c-de-01-0010" num="0010">
<claim-text>Eine Anordnung, die ein Ätzsystem (10) und eine Struktur (40) aufweist, die aus einem Material ist, das selektiv durch das System (10) geätzt werden kann, und ein Erster (42)- und Zweiter (46)-Bereich-Ätzsystem (10) aufweist, mit folgenden Merkmalen:
<claim-text>einer ersten Elektromagnetische-Strahlung-Quelle (20), die konfiguriert ist, um eine erste elektromagnetische Strahlung (24) auf den ersten Bereich (42) der Struktur (40) anzuwenden, wobei die erste elektromagnetische Strahlung (24) ausgewählt ist, um eine Charakteristik des ersten Bereichs (42) zu ändern; und</claim-text>
<claim-text><b>gekennzeichnet durch</b> eine zweite Elektromagnetische-Strahlung-Quelle (30), die konfiguriert ist, um eine zweite elektromagnetische Strahlung (34) auf den zweiten Bereich (46) der Struktur (40) anzuwenden, wobei die zweite elektromagnetische Strahlung (34) konfiguriert ist, um den zweiten Bereich (46) der Struktur (40) selektiv abzutragen.</claim-text></claim-text></claim>
</claims><!-- EPO <DP n="14"> -->
<claims id="claims03" lang="fr">
<claim id="c-fr-01-0001" num="0001">
<claim-text>Procédé de gravure d'une structure (40) comprenant: l'application d'un premier rayonnement électromagnétique (24) sur une première zone (42) d'une structure (40) comprenant une première (42) et une seconde (46) zones, modifiant ainsi une caractéristique physique de la structure (40) dans la première zone (42) ; <b>caractérisé par</b> l'application d'un second rayonnement électromagnétique (34) sur la seconde zone (46) de la structure (40), le second rayonnement électromagnétique (34) étant configuré pour enlever de manière sélective la seconde zone (46) de la structure (40).</claim-text></claim>
<claim id="c-fr-01-0002" num="0002">
<claim-text>Procédé selon la revendication 1, dans lequel ladite modification d'une caractéristique physique de la structure (40) comprend le fait de faire fondre le matériau dans la première zone (42) et, avant l'application du second rayonnement électromagnétique (34), le matériau est laissé se stabiliser.</claim-text></claim>
<claim id="c-fr-01-0003" num="0003">
<claim-text>Procédé selon la revendication 1, où la caractéristique est la cristallinité.</claim-text></claim>
<claim id="c-fr-01-0004" num="0004">
<claim-text>Procédé selon la revendication 3, où l'application du premier rayonnement électromagnétique (24) comprend le fait de faire fondre une couche de surface (40b) dans la zone (42), et le fait<!-- EPO <DP n="15"> --> de laisser la couche de surface (40b) dans la zone (42) se recristalliser.</claim-text></claim>
<claim id="c-fr-01-0005" num="0005">
<claim-text>Procédé selon la revendication 1, où l'application du premier rayonnement électromagnétique (24) comprend l'application d'un premier faisceau laser (24) avec une fluence suffisante pour fusionner une couche de surface (40b) de la structure (40) dans la première zone (42), mais insuffisante pour enlever la couche de surface (40b) de la structure (40) dans la première zone (42).</claim-text></claim>
<claim id="c-fr-01-0006" num="0006">
<claim-text>Procédé selon la revendication 5, où l'application du second rayonnement électromagnétique (34) comprend l'application d'un second faisceau laser (34) avec une fluence suffisante pour enlever la seconde zone (46) de la couche de surface (40b) non fondue par le premier faisceau laser (24), mais insuffisante pour enlever la première zone (42) de la couche de surface (40b).</claim-text></claim>
<claim id="c-fr-01-0007" num="0007">
<claim-text>Procédé selon l'une quelconque des revendications précédentes, comprenant l'utilisation d'un laser YAG pour appliquer le premier rayonnement électromagnétique (34).</claim-text></claim>
<claim id="c-fr-01-0008" num="0008">
<claim-text>Procédé selon l'une quelconque des revendications précédentes, comprenant l'utilisation d'un laser YAG pour appliquer le second rayonnement électromagnétique (34).</claim-text></claim>
<claim id="c-fr-01-0009" num="0009">
<claim-text>Procédé selon l'une quelconque des revendications précédentes, dans lequel l'application du premier rayonnement électromagnétique (24) sur la première zone (42) comprend la mise en place<!-- EPO <DP n="16"> --> d'un masque (50) entre le premier rayonnement électromagnétique (24) et la structure (40), le masque (50) configuré pour protéger la seconde zone (46) de la structure (40) du premier rayonnement électromagnétique (24).</claim-text></claim>
<claim id="c-fr-01-0010" num="0010">
<claim-text>Agencement comprenant un système de gravure (10) et une structure (40) qui est constituée d'un matériau apte à être gravé de manière sélective par le système (10) et comprend un système de gravure d'une première (42) et d'une seconde (46) zones, comprenant : une première source de rayonnement électromagnétique (20) configurée pour appliquer un premier rayonnement électromagnétique (24) sur la première zone (42) de la structure (40), le premier rayonnement électromagnétique (24) étant choisi pour modifier une caractéristique de la première zone (42) ; et <b>caractérisé par</b> une seconde source de rayonnement électromagnétique (30) configurée pour appliquer un second rayonnement électromagnétique (34) sur la seconde zone (46) de la structure (40), le second rayonnement électromagnétique (34) étant configuré pour enlever de manière sélective la seconde zone (46) de la structure (40).</claim-text></claim>
</claims><!-- EPO <DP n="17"> -->
<drawings id="draw" lang="en">
<figure id="f0001" num=""><img id="if0001" file="imgf0001.tif" wi="165" he="212" img-content="drawing" img-format="tif"/></figure><!-- EPO <DP n="18"> -->
<figure id="f0002" num=""><img id="if0002" file="imgf0002.tif" wi="165" he="222" img-content="drawing" img-format="tif"/></figure><!-- EPO <DP n="19"> -->
<figure id="f0003" num=""><img id="if0003" file="imgf0003.tif" wi="148" he="233" img-content="drawing" img-format="tif"/></figure>
</drawings>
<ep-reference-list id="ref-list">
<heading id="ref-h0001"><b>REFERENCES CITED IN THE DESCRIPTION</b></heading>
<p id="ref-p0001" num=""><i>This list of references cited by the applicant is for the reader's convenience only. It does not form part of the European patent document. Even though great care has been taken in compiling the references, errors or omissions cannot be excluded and the EPO disclaims all liability in this regard.</i></p>
<heading id="ref-h0002"><b>Patent documents cited in the description</b></heading>
<p id="ref-p0002" num="">
<ul id="ref-ul0001" list-style="bullet">
<li><patcit id="ref-pcit0001" dnum="US4961052A"><document-id><country>US</country><doc-number>4961052</doc-number><kind>A</kind></document-id></patcit><crossref idref="pcit0001">[0001]</crossref><crossref idref="pcit0003">[0005]</crossref></li>
<li><patcit id="ref-pcit0002" dnum="US4834834A"><document-id><country>US</country><doc-number>4834834</doc-number><kind>A</kind></document-id></patcit><crossref idref="pcit0002">[0004]</crossref></li>
</ul></p>
</ep-reference-list>
</ep-patent-document>
